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Measurements of the branching fractions of Xi_c⁰ to Λ K_S⁰, Xi_c⁰ to Sigma⁰ K_S⁰, and Xi_c⁰ to Sigma^+ K^- decays at Belle

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arxiv 2111.08981 v2 pith:3LKXY3ZH submitted 2021-11-17 hep-ex hep-ph

Measurements of the branching fractions of Xi_c⁰ to Λ K_S⁰, Xi_c⁰ to Sigma⁰ K_S⁰, and Xi_c⁰ to Sigma^+ K^- decays at Belle

Belle collaboration: Y. Li , J. X. Cui , S. Jia , C. P. Shen , I. Adachi , J. K. Ahn , H. Aihara , S. Al Said
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D. M. Asner H. Atmacan T. Aushev R. Ayad V. Babu S. Bahinipati P. Behera K. Belous J. Bennett M. Bessner V. Bhardwaj B. Bhuyan T. Bilka A. Bobrov D. Bodrov G. Bonvicini J. Borah A. Bozek M. Bra\v{c}ko P. Branchini T. E. Browder A. Budano M. Campajola D. \v{C}ervenkov M. C. Chang P. Chang A. Chen B. G. Cheon K. Chilikin H. E. Cho K. Cho S.-J. Cho S. K. Choi Y. Choi S. Choudhury D. Cinabro S. Cunliffe S. Das G. De Nardo G. De Pietro R. Dhamija F. Di Capua J. Dingfelder Z. Dole\v{z}al T. V. Dong D. Dossett D. Epifanov T. Ferber A. Frey B. G. Fulsom R. Garg V. Gaur N. Gabyshev A. Giri P. Goldenzweig T. Gu K. Gudkova C. Hadjivasiliou S. Halder O. Hartbrich K. Hayasaka H. Hayashii M. T. Hedges W. S. Hou C.-L. Hsu T. Iijima K. Inami G. Inguglia A. Ishikawa R. Itoh M. Iwasaki Y. Iwasaki W. W. Ja obs E. J. Jang Y. Jin K. K. Joo J. Kahn A. B. Kaliyar T. Kawasaki C. Kiesling C. H. Kim D. Y. Kim K. H. Kim Y. K. Kim K. Kinoshita P. Kody\v{s} T. Konno A. Korobov S. Korpar E. Kovalenko P. Kri\v{z}an R. Kroeger P. Krokovny T. Kuhr M. Kumar R. Kumar K. Kumara A. Kuzmin Y.-J. Kwon Y. T. Lai T. Lam J. S. Lange M. Laurenza S. C. Lee C. H. Li J. Li L. K. Li Y. B. Li L. Li Gioi J. Libby K. Lieret D. Liventsev A. Martini M. Masuda T. Matsuda D. Matvienko F. Meier M. Merola F. Metzner K. Miyabayashi R. Mizuk G. B. Mohanty R. Mussa M. Nakao Z. Natkaniec A. Natochii L. Nayak M. Nayak M. Niiyama N. K. Nisar S. Nishida K. Ogawa S. Ogawa H. Ono P. Oskin P. Pakhlov G. Pakhlova T. Pang S. Pardi S. H. Park S. Patra S. Paul T. K. Pedlar R. Pestotnik L. E. Piilonen T. Podobnik V. Popov E. Prencipe M. T. Prim M. R\"ohrken A. Rostomyan N. Rout G. Russo D. Sahoo S. Sandilya A. Sangal L. Santelj T. Sanuki V. Savinov G. Schnell C. Schwanda Y. Seino K. Senyo M. E. Sevior M. Shapkin C. Sharma J.-G. Shiu B. Shwartz J. B. Singh A. Sokolov E. Solovieva S. Stani\v{c} M. Stari\v{c} Z. S. Stottler J. F. Strube M. Sumihama T. Sumiyoshi M. Takizawa U. Tamponi K. Tanida F. Tenchini M. Uchida Y. Unno K. Uno S. Uno P. Urquijo Y. Usov R. Van Tonder G. Varner A. Vinokurova E. Waheed E. Wang M. Z. Wang M. Watanabe S. Watanuki O. Werbycka E. Won B. D. Yabsley W. Yan S. B. Yang H. Ye J. Yelton C. Z. Yuan Y. Zhai Z. P. Zhang V. Zhilich V. Zhukova
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classification hep-ex hep-ph
keywords sigmabranchingfractionlambdafractionstimesbelledecays
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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Using the entire data sample of $980\mathrm{~fb}^{-1}$ collected with the Belle detector at the KEKB asymmetric-energy $e^+e^-$ collider, we present measurements of the branching fractions of the Cabibbo-favored decays $\Xi_c^0 \to \Lambda K_S^0$, $\Xi_c^0 \to \Sigma^0 K_S^0$, and $\Xi_c^0 \to \Sigma^+ K^-$. Taking the decay $\Xi_c^0 \to \Xi^- \pip$ as the normalization mode, we measure the branching fraction ratio ${\cal B}(\Xi_c^0 \to \Lambda K_S^0)/{\cal B}(\Xi_c^0 \to \Xi^- \pi^+) = 0.229\pm0.008\pm0.012$ with improved precision, and measure the branching fraction ratios ${\cal B}(\Xi_c^0 \to \Sigma^0 K_S^0)/{\cal B}(\Xi_c^0 \to \Xi^- \pi^+) = 0.038\pm0.006\pm0.004$ and ${\cal B}(\Xi_c^0 \to \Sigma^+ K^-)/{\cal B}(\Xi_c^0 \to \Xi^- \pi^+) = 0.123\pm0.007\pm0.010$ for the first time. Taking into account the branching fraction of the normalization mode, the absolute branching fractions are determined to be ${\cal B}(\Xi_c^0 \to \Lambda K_S^0) = (3.27\pm0.11\pm0.17\pm0.73) \times 10^{-3}$, ${\cal B}(\Xi_c^0 \to \Sigma^0 K_S^0) = (0.54\pm 0.09\pm 0.06\pm 0.12) \times 10^{-3}$, and ${\cal B}(\Xi_c^0 \to \Sigma^+ K^-) = (1.76\pm 0.10\pm0.14\pm 0.39) \times 10^{-3}$. The first and second uncertainties above are statistical and systematic, respectively, while the third ones arise from the uncertainty of the branching fraction of $\Xi_c^0 \to \Xi^- \pi^+$.

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